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References

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  1. H. W. Bode, Network Analysis and Feedback Amplifier Design (Van Nostrand, New York, 1945).
  2. D. M. Roessler, Br. J. Appl. Phys. 16, 119 (1965); Br. J. Appl. Phys. 17, 1313 (1966).
    [CrossRef]
  3. S. Roberts, D. D. Coon, J. Opt. Soc. Am. 52, 1023 (1962).
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  4. W. S. Rodney, R. J. Spindler, J. Opt. Soc. Am. 44, 677 (1954).
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  5. B. Brixner, J. Opt. Soc. Am. 57, 675 (1967).
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  6. E. V. Loewenstein, J. Opt. Soc. Am. 51, 108 (1961).
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  7. E. E. Russell, E. E. Bell, J. Opt. Soc. Am. 57, 542 (1967).
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  8. H. J. Hagemann, W. Gudat, C. Kunz, J. Opt. Soc. Am. 65, 742 (1975).
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  9. D. A. Gryvnak, D. E. Burch, J. Opt. Soc. Am. 55, 625 (1965).
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  10. I. H. Malitson, F. V. Murphy, W. S. Rodney, J. Opt. Soc. Am. 48, 72 (1958).
    [CrossRef]

1975 (1)

1967 (2)

1965 (2)

D. M. Roessler, Br. J. Appl. Phys. 16, 119 (1965); Br. J. Appl. Phys. 17, 1313 (1966).
[CrossRef]

D. A. Gryvnak, D. E. Burch, J. Opt. Soc. Am. 55, 625 (1965).
[CrossRef]

1962 (1)

1961 (1)

1958 (1)

1954 (1)

Bell, E. E.

Bode, H. W.

H. W. Bode, Network Analysis and Feedback Amplifier Design (Van Nostrand, New York, 1945).

Brixner, B.

B. Brixner, J. Opt. Soc. Am. 57, 675 (1967).
[CrossRef]

Burch, D. E.

Coon, D. D.

Gryvnak, D. A.

Gudat, W.

Hagemann, H. J.

Kunz, C.

Loewenstein, E. V.

Malitson, I. H.

Murphy, F. V.

Roberts, S.

Rodney, W. S.

Roessler, D. M.

D. M. Roessler, Br. J. Appl. Phys. 16, 119 (1965); Br. J. Appl. Phys. 17, 1313 (1966).
[CrossRef]

Russell, E. E.

Spindler, R. J.

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Figures (4)

Fig. 1
Fig. 1

Optical constants of fused silica. The ordinate represents either n or k.

Fig. 2
Fig. 2

Optical constants of sapphire. The ordinate represents either n or k.

Fig. 3
Fig. 3

Comparison of current refractive-index data for fused silica with those measured by minimum deviation. The latter make the smooth curve.

Fig. 4
Fig. 4

Comparison of current refractive-index data for sapphire with those measured by minimum deviation. The latter make the smooth curve.

Equations (3)

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n = 1 R 1 + R 2 R cos θ ,
k = 2 R sin θ 1 + R 2 R cos θ .
θ ( ω 0 ) = 1 π 0 ln | ω + ω 0 ω ω 0 | d ln R ( ω ) d ω d ω ,

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